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Volumetric physiological measuring system and method

Inactive Publication Date: 2008-06-24
VOLUSENSE AS
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  • Summary
  • Abstract
  • Description
  • Claims
  • Application Information

AI Technical Summary

Benefits of technology

[0030]Summation of the induced voltages is accomplished by electrical serial connection of the loops, effectively reducing the complexity of the system, since only one voltage needs to be measured. This is an important advantage of the invention disclosed herein resulting in reduced system complexity. The choice of the loop spacing s (also referred interchangeably herein as distance d) is a compromise between accuracy and convenience in the design of the volume transducer. A low value of s means that a higher number of loops will be needed to encompass the measurement region, which typically is from the level of the axilla and down to the crest of the hips, when measuring a torso. If the number of loops becomes high, the self-inductance of the serially connected loops starts to increase dramatically, with implications for the design of the electronic circuits. A preferable embodiment is to use values of s in the range of four to eight cm, which are the smallest values to be used for infants. This typically results in eight (8) to ten (10) loops. Other configurations, however, are possible. The magnetic field need only be homogeneous within the volume occupied by the relevant parts of the patient's body or other object being measured. Practical experience indicates that a field of sufficient intensity and homogeneity can be generated just by arranging a conductor wire as a vertical rectangular loop, following the floor, walls and ceiling of the room, and feeding an alternating current through the loop. Preferable values are 10 kHz to 200 kHz with currents below 1 A, although other configurations are possible. For example, more than one electrical conductor loop may be used.
[0031]FIGS. 2-8 relate to a first embodiment of this invention discussed below. This embodiment, shown in block diagram form in FIG. 2, comprises integrating both the alternating current source for the current loop that generates the magnetic field and the circuits needed to amplify and rectify the returned signal into a single unit. Stable crystal oscillator 30 controls system 20, with the output frequency of the oscillator being divided down to the desired value by binary counter 34. The suggested values of 1 MHz and a division of 16 are arbitrary. It is, however, an advantage that the signal fed into the power amplifier 36 is a symmetric square wave, since this waveform lacks even frequency harmonics. The removal of unwanted harmonic frequency components by filter 37 is then easier. Such removal of harmonics is preferable to avoid radiation interference with other electronic equipment. The amplifier output will eventually be fed into an inductive load that absorbs almost no energy. By using a (class D) switching amplifier design, and by proper design of the low-pass filter, the total power consumption of the amplifier unit can be minimized, reducing the demands for circuit cooling and for power supply capacity. The low-pass filter 37 would likely be a passive one, and would not introduce substantial phase-shifts to the voltage waveform at the frequency used. The signal picked up by the serially-connected loops, which in one embodiment are wrapped around a patient as shown and described below in relation to FIG. 6, is first fed into band pass filter 44. The purpose of this filter is to increase the system noise immunity. The filter can be designed as a narrow-band resonant transformer, effectively implementing galvanic separation of the conductive wires close to the patient and the rest of the apparatus.
[0032]Pre-amplifier 48 is useful since the noise performance of the amplifiers is better than that of demodulator 53. The gain of the amplifier need not be more than necessary to suppress the noise of the demodulator, with a typical value of about 20 to 25 dB.
[0033]The coherent demodulator 53 rectifies the alternating voltage signal, and is easily implemented by CMOS analog switches, such as the CD4016 or CD4066 circuit. Using a coherent demodulator has two advantages. It is very linear over a broad signal intensity range, and together with low-pass filter 58, a substantial improvement in relation to noise suppression is achieved. The effective bandwidth of the amplifier chain will be twice the cut-off frequency of low-pass filter 58, with one example of atypical value of this cut-off frequency being 5 Hz to 15 Hz, with the highest value suited for infants with a higher natural respiration rate.
[0034]The signal-conditioning block 63 serves several purposes. It provides amplification of the signal, making it suited for further processing in a computer-based system. Also, the unit provides some means of coarse adjustment of the amplification, preferably controlled by the analyzing software. Since the signal at the output of the low-pass filter 58 contains a substantial DC or constant component (corresponding to the total volume of the body inside the coils), some means of subtracting this component will increase the sensitivity of the system in detecting small volume changes. Such subtraction can be made with an electronic high-pass filter, the cut-off frequency of which must be substantially below common respiration frequencies (0.05 Hz or below). In order to shorten the time for the output signal to stabilize at start-up of the system, a means of shortening the time constant of this filter (by resistor switching) is desired. In some cases, where slow changes not related to respiration are measured, absolute readouts of volume without any zero subtraction might be desired. Applications of this might be monitoring of edema development, vascular volume reflexes, muscle growth or atrophy, effects of surgical procedures, etc.
[0035]The electronic circuits described above are easily constructed within less than 50 cm2 of circuit board area, and could be integrated with an A / D converter and interface control circuitry on a plug-in board for an ordinary personal computer, for example as shown in FIG. 14 below. A complete stand-alone unit could also be made, with the size and complexity being dependent on the amount of signal analysis, presentation capability and storage capacity built into the unit. It should be emphasized that the above illustrative description is for only one embodiment of the invention, with numerous alternate means of practicing the underlying technology also being within the scope of the appended claims. Parts of the function of the suggested block diagram in FIG. 2 could be implemented using digital signal processing or other means. At least one alternate construction is to let all processing of the received signal be digital from and including demodulator 53 with a sampling rate of exactly twice the loop current frequency.

Problems solved by technology

Unfortunately these measurements are often crude and inaccurate, or at best rely upon outmoded technical modalities or upon unreliable.
For long-term monitoring purposes, the airway-based techniques are inappropriate since they interfere with normal breathing and are unpleasant for the patient.
Although airway-based techniques are currently used in patients dependent on respiratory-assist devices there may be less intrusive and more reliable means of obtaining such data.
Unfortunately, this is not the case for the cross-sectional area variations of the human chest or abdomen that are caused by respiration.
Common to all area-based methods is a considerable uncertainty in the calculations of volume variations from the estimated area variations.
The calibration procedure depends highly upon patient cooperation to obtain coefficients for both chest and abdominal measurement sites, and is virtually inapplicable to small children, patients with dyspnea (shortness of breath), and unconscious patients.

Method used

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  • Volumetric physiological measuring system and method

Examples

Experimental program
Comparison scheme
Effect test

example 1

[0057]A circular electrical conductor loop with a radius of 1.5 meters was placed on the floor. An alternating current of 0.1 A with a frequency of 100 kHz was fed through the conductor from a signal generator. A small, 10×10 cm (100 cm2) square conductor loop was connected to the input of a broadband signal amplifier with a gain of 40 dB, and the output from this amplifier was passed through a narrow 100 kHz band-pass filter with no gain. The output signal from the filter was presented on an oscilloscope screen, where voltages could be read by cursors. When the small loop was positioned flat on the floor in the center of the larger current loop, a voltage of 5 mV p / p was measured. This voltage remained essentially constant when the small loop was elevated 50 cm above the floor, and it also remained constant when the small loop was moved up to 50 cm in any horizontal direction away from the center of the large current loop. Another square loop, measuring 14.1×14.1 cm, with an area o...

example 2

[0058]The same conductor loops as described in Example 1 were used, but the 0.1 A current from the signal generator was fed to the 100 cm2 loop, and the large loop on the floor was connected to the input of the 40 dB broadband amplifier. The small loop was positioned as explained in Example 1. The same general relations between induced voltage and loop position and area was observed as in Example 1, however the voltages were reduced to 250 μV when using the 100 cm2 loop, and 500 μV when using the 200 cm2 loop.

example 3

[0059]Referring to FIG. 11, three identical cylindrical ferrite rods 175 with a diameter of 8 mm, length of 150 mm and permeability of 100 were arranged along a straight horizontal line with a common axis. The end-to-end horizontal spacing between each rod was 50 cm. The two outer coils were equipped with 163 turns of lacquer-insulated 0.1 mm copper wire evenly distributed along a central 8 cm segment of the rod, while the center rod had 100 turns arranged in the same manner. The coils were electrically connected in series, and care was taken to assure identical current directions in all coils. The serially connected coils were then tuned to parallel resonance at 100 kHz with a common capacitor 177 of about 10 nF. An oscilloscope directly monitored the signal from the resonant circuit. A 10 cm×10 cm current loop carrying a 100 kHz alternating current of 0.1 A was positioned adjacent to the coil assembly, keeping the orientation of the loop perpendicular to the ferrite rods common ax...

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Abstract

A system and method for measuring volumes and areas using electromagnetic induction techniques. A current is generated and fed into one of two coil assemblies to induce voltage into another coil assembly to provide accurate values for volume or area.

Description

CROSS-REFERENCE TO RELATED APPLICATION[0001]This application is a continuation-in-part of U.S. Divisional patent application Ser. No. 10 / 087,302, filed Feb. 28, 2002, now U.S. Pat. No. 6,945,941, which in turn is an application of U.S. patent application Ser. No. 09 / 428,358, filed Oct. 28, 1999, now U.S. Pat. No. 6,374,667, issued Apr. 23, 2002, which is incorporated herein by reference.FIELD OF THE INVENTION[0002]The invention relates to a system and method for accurate measurements of volume and area of objects, utilizing electromagnetic induction techniques.BACKGROUND OF THE INVENTION[0003]Numerous opportunities exist in which accurate measurements of volume and area are essential, particularly of objects or portions of objects having variable volumes or areas. For example, in the field of medicine, the recording of breathing volumes in patients is often quite critical. Unfortunately these measurements are often crude and inaccurate, or at best rely upon outmoded technical modali...

Claims

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Application Information

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IPC IPC(8): A61B5/103A61B5/08A61B5/117G01F1/56G01F1/58G01F1/716G01N27/72G01P5/08G01R33/00G01R33/02G01R33/12A61B5/053A61B5/06A61B5/113
CPCA61B5/0535A61B5/06A61B5/1135A61B5/1073A61B5/062
Inventor ERIKSEN, MORTENERIKSEN, ERIK
Owner VOLUSENSE AS
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